Search results for "Fission"

showing 10 items of 421 documents

Evidence for quasi-fission in40Ar+208Pb collisions near the coulomb-barrier

1987

Fission-fragment angular distributions were measured in the reaction of40Ar with208Pb near the fusion barrier. For nearly symmetric mass-/charge splits we find angular distributions symmetric around θ=90 degrees, however, with unusually large anisotropies. These develop gradually into forward-backward asymmetric distributions as one moves away from mass-/charge symmetry. This indicates that non-compound fission (‘quasi-fission’) competes with true fusion-fission. The relative contribution of quasi-fission to the total fission cross section is somewhere between 51 and 85%. In the framework of the extra-push model this is equivalent to an extra-extra push energy for compound-nucleus formation…

Nuclear and High Energy PhysicsFissionChemistryNuclear TheoryCoulomb barrierCharge (physics)Symmetry (physics)Nuclear physicsCross section (physics)Saddle pointNuclear fusionAtomic physicsNuclear ExperimentParametrizationZeitschrift f�r Physik A Atomic Nuclei
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Beta-decay of148,150,152Pr into levels of148,150,152Nd

1988

Theβ−-decay of148,150,152Pr into levels of148,150,152Nd has been studied byγ-singles,γγ-coincidence and for148Pr also byγγ-angular correlation measurements. The praseodymium activities have been obtained by thermal neutron-induced fission of235U followed by on-line mass separation with the helium-jet coupled mass separator HELIOS. Decay schemes for these heaviest praseodymium nuclides are proposed. From the angular correlation measurements spin values for the seven lowest levels of148Nd are deduced. Spin and parity assignments for the lower levels in150,152Nd have been extrapolated from level systematics.

Nuclear and High Energy PhysicsFissionChemistryPraseodymiumThermalchemistry.chemical_elementNuclear fusionParity (physics)NuclideAtomic physicsMass separationBeta decayZeitschrift f�r Physik A Atomic Nuclei
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Low-spin excitations in the 109Tc nucleus

2012

Monoisotopic samples of ${}^{109}$Mo nuclei, produced in the deuteron-induced fission of ${}^{238}$U and separated using the IGISOL mass separator coupled to a Penning trap, were used to perform $\ensuremath{\beta}$- and $\ensuremath{\gamma}$-coincidence spectroscopy of ${}^{109}$Tc. Spin and parity 5/2${}^{+}$ for the ground state of ${}^{109}$Mo, proposed earlier, are supported in the present work. Three new low-energy levels observed in ${}^{109}$Tc are interpreted as bandheads of the $\ensuremath{\pi}3/{2}^{\ensuremath{-}}$[301], $\ensuremath{\pi}5/{2}^{\ensuremath{-}}$[303], and $\ensuremath{\pi}1/{2}^{+}$[431] configurations, respectively. A further three levels observed around 0.4 Me…

Nuclear and High Energy PhysicsFissionProlate spheroid[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]kiihdytinpohjainen fysiikka01 natural sciencesydinrakenneDouble beta decay0103 physical sciencesmedicine010306 general physicsSpectroscopynuclear spectroscopyPhysicsta114accelerator-based physics010308 nuclear & particles physicsParity (physics)medicine.anatomical_structurenuclear structureydinspektroskopiaAtomic physicsydinfysiikkaGround stateNucleusExcitation
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Laser photodetachment of radioactive $^{128}$I$^−$

2017

International audience; The first experimental investigation of the electron affinity (EA) of a radioactive isotope has been conducted at the CERN-ISOLDE radioactive ion beam facility. The EA of the radioactive iodine isotope (128)I (t (1/2) = 25 min) was determined to be 3.059 052(38) eV. The experiment was conducted using the newly developed Gothenburg ANion Detector for Affinity measurements by Laser PHotodetachment (GANDALPH) apparatus, connected to a CERN-ISOLDE experimental beamline. (128)I was produced in fission induced by 1.4 GeV protons striking a thorium/tantalum foil target and then extracted as singly charged negative ions at a beam energy of 20 keV. Laser photodetachment of th…

Nuclear and High Energy PhysicsIon beamFissionPhysics::Instrumentation and Detectors[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]02 engineering and technologyPhoton energy01 natural sciences7. Clean energySecondary electronsISOLDElaw.inventionIonlawElectron affinity0103 physical scienceselectron affinityPhysics::Atomic Physics010306 general physicsNuclear ExperimentPhysicsiodinephotodetachment021001 nanoscience & nanotechnologyLaserAccelerators and Storage RingsBeamlinePhysics::Accelerator PhysicsAtomic physics0210 nano-technology
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Production of neutron-rich surface-ionized nuclides at PARRNe

2002

Yields of neutron-rich isotopes produced by fast neutron induced fission of 238 U were measured at the ISOL set-up Production dAtomes Radioactifs Riches en Neutrons. A surface ion source was used to ionize selectively elements with low ionization potentials. In order to observe also the most n-rich isotopes, the identification was achieved by a combined measurement of b- and c-rays and b-delayed neutrons. The flux of fast neutrons inducing fission was generated by a 1 lA beam of 26 MeV deuterons stopped in a graphite converter. The target was a standard ISOLDE type 238 UC

Nuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsChemistryFissionAstrophysics::High Energy Astrophysical PhenomenaIsotopes of samariumNuclear TheoryRadiochemistry[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesIon sourceNeutron temperatureNuclear physics0103 physical sciencesNeutronNuclideNuclear Experiment010306 general physicsInstrumentationIsotopes of caesium
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The ion-guide isotope separator on-line at the Tohoku University Cyclotron

1987

Abstract The status of the ion-guide isotope separator on-line at the Tohoku University Cyclotron is reported. The optimum ion-guide parameters were determined from test experiments using atomic and molecular ions ionized with an electric discharge inside the target chamber as well as using 64 Ga(T 1 2 = 2.6 m ) ions produced by the 64Zn(p, n) reaction. Using the present system together with a ΔE−E plastic counter telescope and a germanium detector we identified 16 short-lived nuclei including the first mass-separated nuclei 57Cu and 45V. The efficiency of mass separation for 64Ga was ϵ ∼ 1%, where ϵ is defined as the number of atoms collected at the end of the separator divided by that rec…

Nuclear and High Energy PhysicsIsotopeCyclotronAnalytical chemistrychemistry.chemical_elementUraniumIonlaw.inventionSemiconductor detectorNuclear physicschemistrylawNuclear fissionIonizationElectric dischargeInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Isotope shift and hyperfine structure measurements at the242f Am fission isomer

1996

Istope shift and hyperfine structure measurements have been performed for the242fAm fission isomer with target production rates of only a few per second. The method is based on resonance ionization spectroscopy (RIS) in a buffer gas cell with radioactive decay detection of the ionization process (RADRIS). A relative isotope shift ratioX exp=IS242f,241/ IS243,241=41.7±0.9 has been measured for the 500.02 nm transition corresponding to a nuclear parameter Λ242f,241=5.4±0.3 fm2. The analysis of the quadrupole moment based on the deformed Fermi-model of the nuclear charge distribution including second order corrections results inQ 20=38.2 ±1.4( −0.8 +0.4 )model eb. The measurement of the hyperf…

Nuclear and High Energy PhysicsIsotopeFissionChemistryCondensed Matter PhysicsAtomic and Molecular Physics and OpticsEffective nuclear chargeIsomeric shiftIsotopic shiftIonizationPhysical and Theoretical ChemistryAtomic physicsHyperfine structureRadioactive decayHyperfine Interactions
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High-accuracy mass spectrometry of fission products with Penning traps

2012

Mass measurements of fission products based on Penning-trap technique are reviewed in this article. More than 300 fission products have been measured with JYFLTRAP, ISOLTRAP, CPT, LEBIT and TITAN Penning traps with a typical precision of δm/m ≈ 10−7 − 10−8. In general, the results agree well with each other. The new data provide a valuable source of information and a challenge for the future development of theoretical mass models as well as for obtaining a deeper insight into microscopic properties of atomic nuclei as measured, for example, via key mass differentials. Shape transitions around N = 60, subshell closure at N = 40 and shell closures at N = 50 and N = 82 have been investigated i…

Nuclear and High Energy PhysicsNuclear TheoryMass spectrometry01 natural sciencesISOLTRAPkiihdytinpohjainen fysiikkaNuclear physicssymbols.namesakeydinrakenne0103 physical sciencesNuclear astrophysics010306 general physicsNuclear ExperimentPhysicsnuclear spectroscopyFission products010308 nuclear & particles physicsaccelerator-based physicsNuclear structure13. Climate actionPairingAtomic nucleusnuclear structuresymbolsydinspektroskopiaAtomic physicsTitan (rocket family)ydinfysiikka
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The neutron background of the XENON100 dark matter search experiment

2013

TheXENON100 experiment, installed underground at the LaboratoriNazionali del Gran Sasso, aims to directly detect dark matter in the form of weakly interacting massive particles (WIMPs) via their elastic scattering off xenon nuclei. This paper presents a study on the nuclear recoil background of the experiment, taking into account neutron backgrounds from (alpha, n) reactions and spontaneous fission due to natural radioactivity in the detector and shield materials, as well as muon-induced neutrons. Based on MonteCarlo simulations and using measured radioactive contaminations of all detector components, we predict the nuclear recoil backgrounds for the WIMP search results published by theXENO…

Nuclear and High Energy PhysicsParticle physicsLarge Underground Xenon experimentPhysics::Instrumentation and DetectorsDark matterGeant4Astrophysics::Cosmology and Extragalactic AstrophysicsWIMP Argon Programme01 natural sciencesNuclear physicsWIMPNuclear and High Energy Physics Neutron Background Dark Matter Search XENON TPC0103 physical sciencesNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSSpontaneous fissionPhysicsElastic scatteringFluxMuons010308 nuclear & particles physicsAstrophysics::Instrumentation and Methods for AstrophysicsDetectorsWeakly interacting massive particlesHigh Energy Physics::ExperimentSimulation
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A facility for production and laser cooling of cesium isotopes and isomers

2018

We report on the design, installation, and test of an experimental facility for the production of ultra-cold atomic isotopes and isomers of cesium. The setup covers a broad span of mass numbers and nuclear isomers, allowing one to directly compare chains of isotopes and isotope/isomer pairs. Cesium nuclei are produced by fission or fusion-evaporation reactions using primary proton beams from a 130 MeV cyclotron impinging upon a suitable target. The species of interest is ejected from the target in ionic form, electrostatically accelerated, mass separated, and routed to a science chamber. Here, ions are neutralized by implantation in a thin foil, and extracted by thermal diffusion. A neutral…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsProtonCesium IsotopesAtomic Physics (physics.atom-ph)FissiontutkimuslaitteetCyclotronFOS: Physical scienceschemistry.chemical_element7. Clean energy01 natural sciencesPhysics - Atomic Physicslaw.inventionIonlaser coolinglawLaser cooling0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentInstrumentationPhysicsultra-cold nucleita114Isotope010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)3. Good healthchemistryCaesiumAtomic physicsydinfysiikkaisotopes and isomersNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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